Spin-galvanic effect due to optical spin orientation
| dc.creator | Ganichev, S. D. | |
| dc.creator | Schneider, Petra | |
| dc.creator | Bel'kov, V. V. | |
| dc.creator | Ivchenko, E. L. | |
| dc.creator | Tarasenko, S. A. | |
| dc.creator | Wegscheider, W. | |
| dc.creator | Weiss, D. | |
| dc.creator | Schuh, D. | |
| dc.creator | Murdin, B. N. | |
| dc.creator | Phillips, P. J. | |
| dc.creator | Pidgeon, C. R. | |
| dc.creator | Clarke, D. G. | |
| dc.creator | Merrick, M. | |
| dc.creator | Murzyn, P. | |
| dc.creator | Beregulin, E. V. | |
| dc.creator | Prettl, W. | |
| dc.date | 2003-03-11 | |
| dc.date | 2003-06-06 | |
| dc.date.accessioned | 2026-07-07T02:50:07Z | |
| dc.date.available | 2026-07-07T02:50:07Z | |
| dc.description | Under oblique incidence of circularly polarized infrared radiation the spin-galvanic effect has been unambiguously observed in (001)-grown $n$-type GaAs quantum well (QW) structures in the absence of any external magnetic field. Resonant inter-subband transitions have been obtained making use of the tunability of the free-electron laser FELIX. It is shown that a helicity dependent photocurrent along one of the $<110>$ axes is predominantly contributed by the spin-galvanic effect while that along the perpendicular in-plane axis is mainly due to the circular photogalvanic effect. This strong non-equivalence of the [110] and [1$\bar{1}$0] directions is determined by the interplay between bulk and structural inversion asymmetries. A microscopic theory of the spin-galvanic effect for direct inter-subband optical transitions has been developed being in good agreement with experimental findings. | |
| dc.identifier | https://arxiv.org/abs/cond-mat/0303193 | |
| dc.identifier | http://arxiv.org/abs/cond-mat/0303193 | |
| dc.identifier.uri | http://salesiana.dossiersoluciones.com/handle/123456789/21002 | |
| dc.subject | Condensed Matter | |
| dc.title | Spin-galvanic effect due to optical spin orientation | |
| dc.type | text |